Well Screen Entrance Velocity

Also known as screen open area · slot velocity · 0.1 ft per second · screen design · incrustation · well screen sizing

Ve=QπDLPV_e = \frac{Q}{\pi \, D \, L \, P}

Enter your known values, leave one input blank, and solves for the missing one. Try different units for next level excitement!

Learning zone

A well screen is not a hole, it is an area. The water entering it has to pass through whatever fraction of the screen's cylindrical surface is actually slot, and the velocity through that open area is Ve=Q/(πDLP)V_e = Q/(\pi D L P). The long-standing design limit is 0.03 m/s, or 0.1 ft/s, a figure Walton fitted to field performance and Driscoll made standard. It is not a physical boundary but an empirical one, and the reasons behind it are all about what happens above it rather than what happens below.

Three things go wrong at high entrance velocity, and they compound each other. Head loss through the slots rises with the square of velocity, which is precisely the CQ2CQ^{2} term on the step-drawdown page, so the well's efficiency falls. Fines that a properly designed filter pack would leave in place get dragged through the slots instead, and the well pumps sand. And the pressure drop across the slots causes dissolved carbon dioxide to come out of solution and dissolved iron to oxidise right at the slot face, so carbonate and iron oxide plate onto the openings rather than staying in the formation. That reduces the open area, which raises the velocity, which accelerates the incrustation. Wells fail this way slowly and then all at once.

The open-area fraction is the number a driller can most easily change and the one most often left to chance. Torch-cut or machine-slotted pipe gives about 3 to 8 per cent open area. Continuous-slot wire-wrapped screen gives 15 to 40 per cent, five to ten times as much, in the same diameter and the same length. If a well cannot make its design rate cleanly, the screen type is usually the first thing to look at, well before anyone reaches for a bigger pump.

Of the three geometric levers, length is nearly always the best buy. Doubling the diameter halves the entrance velocity but requires a larger borehole for the entire depth of the well, which costs real money. Doubling the screen length halves the velocity too, costs only the extra screen, and screens twice as much aquifer while doing it. The standard error on this page is entering the total screen length rather than the length actually opposite saturated, productive aquifer. Screen sitting in a clay interbed or above the water table contributes nothing and should not be in the number.

Well Screen Entrance Velocity
Ve=QπDLPV_e = \frac{Q}{\pi \, D \, L \, P}
QVeDLP
Where
  • VeV_e= Entrance velocity (m/s)
  • QQ= Pumping rate (m³/h)
  • DD= Screen outside diameter (mm)
  • LL= Screen length (m)
  • PP= Open-area fraction